What is and to which end does one study Bohmian Mechanics?
... • the empirical import of BM comes solely from mathematical analysis • Boltzmann’s statistical analysis of BM (ρ = |ϕ|2 ) based on typicality ...
... • the empirical import of BM comes solely from mathematical analysis • Boltzmann’s statistical analysis of BM (ρ = |ϕ|2 ) based on typicality ...
1.2.8. Additional solutions to Schrödinger`s equation
... Figure 1.2.17 Potential and electron wavefunction for an infinitely deep well within an electric field. Since the wave function must be zero at both boundaries, these boundaries must coincide with two different zeros of the Airy function. Since the zeros are discreet rather than continuous our solut ...
... Figure 1.2.17 Potential and electron wavefunction for an infinitely deep well within an electric field. Since the wave function must be zero at both boundaries, these boundaries must coincide with two different zeros of the Airy function. Since the zeros are discreet rather than continuous our solut ...
A scheme for efficient quantum computation with linear optics
... the modes to be used. The basic element that adds photons to the initial state is a single photon source. It can be used to set the state of any given mode to the one-photon state |1i. It is suf®cient to be able to prepare this state non-deterministically. This means that the state preparation has a ...
... the modes to be used. The basic element that adds photons to the initial state is a single photon source. It can be used to set the state of any given mode to the one-photon state |1i. It is suf®cient to be able to prepare this state non-deterministically. This means that the state preparation has a ...
Matthew Neeley, , 722 (2009); DOI: 10.1126/science.1173440
... |0〉) to tunnel out of the well. An on-chip superconducting quantum interference device (SQUID) detects this tunneling (24). For qudit operation, anharmonicity is again crucial because it ensures that all transition frequencies wn,n−1 = (En − En−1)/ħ are distinct, allowing frequency-selective control ...
... |0〉) to tunnel out of the well. An on-chip superconducting quantum interference device (SQUID) detects this tunneling (24). For qudit operation, anharmonicity is again crucial because it ensures that all transition frequencies wn,n−1 = (En − En−1)/ħ are distinct, allowing frequency-selective control ...
Building a Microwave Antenna for a Quantum Microscope
... state will be pumped to the excited state. They will emit a photon and return to the ground state. • A photodiode will be used to be detect these photons. • To observe the Rabi flopping, we will run the experiment, measure, reset, and run again. ...
... state will be pumped to the excited state. They will emit a photon and return to the ground state. • A photodiode will be used to be detect these photons. • To observe the Rabi flopping, we will run the experiment, measure, reset, and run again. ...
Charge dynamics and spin blockade in a hybrid double quantum dot
... The nanowire transistor device, sketched in Fig. 1(a), is fully compatible with the CMOS industry. It is fabricated from an silicon on insulator substrate composed of a 145-nm buried oxide layer and a 11-nm-thick silicon layer doped with phosphorus at a concentration of 5 × 1017 cm−3 . The doped sil ...
... The nanowire transistor device, sketched in Fig. 1(a), is fully compatible with the CMOS industry. It is fabricated from an silicon on insulator substrate composed of a 145-nm buried oxide layer and a 11-nm-thick silicon layer doped with phosphorus at a concentration of 5 × 1017 cm−3 . The doped sil ...
(2)
... the dynamics of an ensemble of trajectories is followed to represent the coupled evolution of the quantum system and bath. Typically, the classical degrees of freedom evolve by Newton’s equations of motion on adiabatic energy surfaces; the evolution is interrupted by ‘‘hops’’ to other adiabatic surf ...
... the dynamics of an ensemble of trajectories is followed to represent the coupled evolution of the quantum system and bath. Typically, the classical degrees of freedom evolve by Newton’s equations of motion on adiabatic energy surfaces; the evolution is interrupted by ‘‘hops’’ to other adiabatic surf ...
Angle Matrix Elements
... not well known. The version given here is from Jackson, Classical Electrodynamics, 2nd Ed., Eq. (3.70). The whole point of this formula is to separate the variables of particle 1 from the variables of particle 2. Once that has been done it is easy to evaluate angular matrix elements. That is, we nee ...
... not well known. The version given here is from Jackson, Classical Electrodynamics, 2nd Ed., Eq. (3.70). The whole point of this formula is to separate the variables of particle 1 from the variables of particle 2. Once that has been done it is easy to evaluate angular matrix elements. That is, we nee ...
Semiclassical approximation of excitations in spin-1 Heisenberg antiferromagnets
... The above model is also known as the Rotor Model. At g = 0 we get a perfectly ordered state with anti-ferromagnetic coupling. Non zero g destroys ordering. It can be proved that even for small values of g the effective contribution to the Hamiltonian due to the second term is very small and thus can ...
... The above model is also known as the Rotor Model. At g = 0 we get a perfectly ordered state with anti-ferromagnetic coupling. Non zero g destroys ordering. It can be proved that even for small values of g the effective contribution to the Hamiltonian due to the second term is very small and thus can ...